{"id":935,"date":"2014-02-17T15:46:45","date_gmt":"2014-02-17T20:46:45","guid":{"rendered":"https:\/\/my.dev.vanderbilt.edu\/mcml\/?page_id=935"},"modified":"2014-02-17T15:46:45","modified_gmt":"2014-02-17T20:46:45","slug":"multiscale-modeling-of-random-nano-and-micro-fiber-reinforced-cementitious-composites-2","status":"publish","type":"page","link":"https:\/\/my.dev.vanderbilt.edu\/mcml\/cv\/multiscale-modeling-of-random-nano-and-micro-fiber-reinforced-cementitious-composites-2\/","title":{"rendered":"Multiscale Modeling of Random Nano- and Micro-Fiber Reinforced Cementitious Composites"},"content":{"rendered":"<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Research Sponsor: <\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: small\"> Vanderbilt University Grant Research Program <\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: small\"> Vanderbilt University Institute for Software Integrated Systems (ISIS) <\/span><\/li>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Investigators: <\/span><\/h4>\n<p><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: small\"> Matthew G. Pike and Caglar Oskay <\/span><br \/>\n<!--...................................................................................--><\/p>\n<h2>Research Goals and Methods<\/h2>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Goals:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">To gain a fundamental understanding of the interactions between the fibers and the cement matrix in carbon nano- and micro-fiber reinforced cement composites<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">To evaluate the effects of the chemical structure of the interface on the macroscopic mechanical failure properties<\/span><\/li>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Multiscale Computational Framework:<\/span><\/h4>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Composite response controlled at the molecular scale through the chemical and mechanical interactions<\/span><\/li>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Nanoscale investigations and nanoscopically informed embedded cohesive law<\/span><\/li>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Link the material microstructure to the composite mesoscale: based on the overall response of the RVE<\/span><\/li>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Computational Design of Carbon Nano- and Micro-Fiber Reinforced Cementitious Composites:<\/span><\/h4>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Random short fiber reinforced composite material<\/span><\/li>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">The inter-facial interaction between the matrix and the reinforcement has significant effect on the overall response of the composite structure<\/span><\/li>\n<li><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\"> Use of the extended finite element method (X-FEM)to model the fibers in the matrix<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Multiscalesummary_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Multiscalesummary_pike.png\" alt=\"\" width=\"700\" \/><\/a><br \/>\n<!--...................................................................................--><\/p>\n<h2>Modeling Short Fibers Reinforced Composites Using XFEM<\/h2>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Representative Volume Element (RVE):<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Constitutive response of the cohesive zone model for interdependent damage-plasticity modeling of the cement phase<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Random short-fiber reinforced matrix idealization<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">XFEM framework to evaluate the response of the RVE<\/span><\/li>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Extended Finite Element Method (XFEM):<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Fibers accounted for by using additional enrichment functions <\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\"> Enrichment of the finite element approximation by additional functions that model the internal boundaries<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Fibers can be modeled as rigid or flexible<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/xfemequation_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/xfemequation_pike.png\" alt=\"\" height=\"75\" \/><\/a><\/p>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Complex finite element discretizations that require resolution of fibers are eliminated<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">N(<strong>x<\/strong>): nodal enrichment function, <strong>u\u0302<\/strong>: nodal value, \u03c8(<strong>x<\/strong>): enrichment function, <strong>c\u0302<\/strong>: additional degree of freedom nodal value<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/xfemelements_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/xfemelements_pike.png\" alt=\"\" width=\"700\" \/><span>XFEM Element Types<\/span><\/a><\/p>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Nodal Enrichment Function:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Enrichment function of fiber inclusion comprised of level set functions<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\"> Level set functions for fiber interface and fiber tips separately<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/enrichmentequation_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/enrichmentequation_pike.png\" alt=\"\" height=\"75\" \/><\/a><\/p>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">\u03a6<sub>\u03b1<\/sub>(<strong>x<\/strong>)=(<strong>x<\/strong>&#8211;<strong>x<\/strong><sub>i<\/sub>)\u00b7<strong>t<\/strong> :  level set function at fiber tip, i &#8211; tracks the motion of each fiber tip<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">\u03a6<sub>c<\/sub>(<strong>x<\/strong>)=min ||<strong>x<\/strong>&#8211;<strong>x<\/strong><sub>r<\/sub>|| :  level set function at interface &#8211; tracks the motion of the fiber interface<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Enrichment_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Enrichment_pike.png\" alt=\"\" width=\"700\" \/><span>Enrichment Function<\/span><\/a><br \/>\n<a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/enrichmentnodes_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/enrichmentnodes_pike.png\" alt=\"\" width=\"700\" \/><span>Enriched Nodal Basis Functions<\/span><\/a><br \/>\n<!--...................................................................................--><\/p>\n<h2>Fiber Response<\/h2>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Rigid Fibers:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Assume each fiber moves as a rigid body as does not deform<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Described through rotation and translation<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Penalty method applied to fiber constraint at fiber\/matrix interface<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/rigidgraph_pike.png.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/rigidgraph_pike.png\" alt=\"\" width=\"700\" \/><\/a><\/p>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Flexible Fibers:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Assume each fiber is flexible and do not bend but stretch under loading<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Flexibility of fiber decrease the strength of the matrix<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">The energy from the stretch is added to the system<\/span><\/li>\n<p><a href=\"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-content\/uploads\/sites\/246\/2014\/02\/stretchgraph1_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/stretchgraph2_pike.png\" alt=\"\" width=\"700\" \/><\/a><br \/>\n<!--...................................................................................--><\/p>\n<h2>Fiber De-Bonding and Cohesive Embedded Laws<\/h2>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Fiber De-Bonding:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Fibers will de-bond from the matrix once the loading reaches a critical stress<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Additional term added to discretization at account for the de-bonding:<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/debondequation_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/debondequation_pike.png\" alt=\"\" height=\"75\" \/><\/a><br \/>\n<a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/debondequation2_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/debondequation2_pike.png\" alt=\"\" height=\"75\" \/><\/a><br \/>\n<a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Debondenrichment_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/Debondenrichment_pike.png\" alt=\"\" width=\"700\" \/><span>De-Bonding Enrichment Function<\/span><\/a><\/p>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Cohesive Embedded Law:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Energy based, nanoscopically informed cohesive embedded law<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Separation over the interface of the fiber and matrix, resisted by cohesive tractions<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Non linear constitutive relationship between cohesive tractions and the displacement jumps along the fiber cement interface as a function of the molecular structure<\/span><\/li>\n<p><a href=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/tractioncurve_debond_pike.png\"><br \/>\n<img decoding=\"async\" class=\"aligncenter size-full wp-image-119\" src=\"https:\/\/cdn-dev.vanderbilt.edu\/t2-my-dev\/wp-content\/uploads\/sites\/246\/2014\/02\/tractioncurve_debond_pike.png\" alt=\"\" width=\"700\" \/><span>Cohesive Traction relationship and Fiber De-Bonding Motion<\/span><\/a><br \/>\n<!--...................................................................................--><\/p>\n<h2>Summary<\/h2>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Multiscale Computational Framework for Modeling the Mechanical Response of Nano- and Micro-Fiber Reinforced Cementitious Composites:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">An efficient XFEM approach is proposed to evaluate the RVE response<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Nano- and micro-fibers modeled for rigid, flexibility and de-bonding of fibers<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Nanoscale response with the nanoscopically informed cohesive embedded law<\/span><\/li>\n<h4><span style=\"font-family: Baskerville,Georgia,Arial,Garamond;font-size: 18px\">Future Potential:<\/span><\/h4>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\">Pathway to achieve simulation based molecular scale engineering of cementitious composites<\/span><\/li>\n<li><span style=\"color: black;font-family: Baskerville,Georgia,Arial,Garamond;font-size: 16px\"> Aid in the composite material design process<\/span><\/li>\n","protected":false},"excerpt":{"rendered":"<p>Research Sponsor: Vanderbilt University Grant Research Program Vanderbilt University Institute for Software Integrated Systems (ISIS) Investigators: Matthew G. Pike and Caglar Oskay Research Goals and Methods Goals: To gain a fundamental understanding of the interactions between the fibers and the cement matrix in carbon nano- and micro-fiber reinforced cement composites To evaluate the effects of&#8230;<\/p>\n","protected":false},"author":235,"featured_media":0,"parent":5,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"tags":[],"class_list":["post-935","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/pages\/935","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/users\/235"}],"replies":[{"embeddable":true,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/comments?post=935"}],"version-history":[{"count":114,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/pages\/935\/revisions"}],"predecessor-version":[{"id":1067,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/pages\/935\/revisions\/1067"}],"up":[{"embeddable":true,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/pages\/5"}],"wp:attachment":[{"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/media?parent=935"}],"wp:term":[{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/my.dev.vanderbilt.edu\/mcml\/wp-json\/wp\/v2\/tags?post=935"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}